Method and laser for breaking limitation of fluorescence spectrum on laser wavelength

ABSTRACT

A method and a laser for breaking through the limitation of fluorescence spectrum on laser wavelength is disclosed. The method includes: exciting electrons to a high energy level by pump light, and suppressing an oscillation of radiation light by laser cavity coating, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, wherein the laser cavity includes an incident mirror, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the laser gain medium is located between an incident mirror and a folding mirror in the laser resonator, and the tuning element is arranged in the laser cavity at a Brewster angle.

This patent application is a continuation application of PCT/CN2022/114666, filed on Aug. 25, 2022, which claims the benefit and priority of Chinese Patent Application No. 202210959521.4, filed on Aug. 10, 2022, the disclosure of which is incorporated by reference herein in its entirety as part of the present application.

TECHNICAL FIELD

The present disclosure relates to the field of laser technology, and more particularly to a method and a laser for breaking the limitation of fluorescence spectrum on laser wavelength.

BACKGROUND ART

Laser, as an important artificial light source, plays an important role in key fields of national economy and national security. Different applications require different wavelengths of laser, and the available laser wavelength depends on the energy level difference of the electron transition. According to Bohr's hydrogen atom model, the energy level of electrons is quantized and discrete, and its spectrum can be broadened to a certain extent due to the influence of uniform and non-uniform broadening. The wavelength of the generated laser can be continuously adjusted in a certain range by the tunable laser technology. In order to expand the laser wavelength, nonlinear optics and frequency conversion technology have been developed. On the basis of the laser emission wavelength, the technology has been extended to many ultraviolet and infrared bands, which meets many practical application requirements. However, the basis of its expansion is still the wavelength of laser, and nonlinear optics and frequency conversion technology are based on the high-order response of electrons in materials to external light field, and the frequency conversion process depends on the nonlinear polarizability of materials. The polarizability is often several orders of magnitude smaller than the linear polarizability, which requires a larger power density of the incident light field; the efficiency of nonlinear frequency conversion also depends on the influence and limitation of phase matching, walk-off, temperature, etc., which requires higher design and application of wavelength extension devices. Therefore, directly expanding the laser wavelength from the process of laser emission and realizing the quantum “cutting” of the electronic transition process have incomparable advantages over the nonlinear frequency conversion technology, at the same time, it can also provide a basic light source for nonlinear optics and frequency conversion technology, and further expand the laser wavelength.

However, as described in Bohr's hydrogen atom model, the quantum orbital of the electron determines the separation of the fluorescence spectrum and also limits the laser wavelength obtained. Therefore, how to break through the fluorescence spectrum limit to obtain a new wavelength laser has been a key technical problem in this field.

SUMMARY

In view of the above, the present disclosure provides a method and a laser for breaking through the limitation of fluorescence spectrum on laser wavelength to solve the technical problems in the background art.

To achieve the above purpose, the present disclosure provides the following technical scheme:

In one aspect, that present disclosure disclose a method of breaking the limit of a fluorescence spectrum on a laser wavelength, the method includes: in a laser gain medium, exciting electrons to a high energy level by pump light, and suppressing an oscillation of radiation light by laser cavity coating; at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, wherein the laser cavity includes an incident mirror, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the laser gain medium is located between an incident mirror and a folding mirror in the laser resonator.

Preferably, the laser gain medium transits electrons to high energy level under the excitation of pump light, specifically including:

focusing the pump light provided by the pump source by a focusing system and then injecting into the laser gain medium to excite the electron transition to the high energy level.

laser resonance is used to enhance a transition probability of an electron-phonon coupling from high-energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of penetrating fluorescence spectrum and realize the oscillation of radiation light, specifically including:

focusing the pump light provided by the pump source by a focusing system and then injecting into the laser gain medium to excite the electron transition to the high energy level.

The laser resonance is used to enhance a transition probability of an electron-phonon coupling from high-energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of penetrating fluorescence spectrum and the oscillation of radiation light, which specifically includes as follows.

When the pump light wavelength is 976 nm, the laser gain medium including a crystal of calcium rare earth borate doped with ytterbium ions with a concentration of 1 at %-30 at %, and the crystal surface of the laser gain medium is polished and plated with a dielectric film with a high transmittance in the wavelength range of 1000 nm-1500 nm;

inputting a mirror plating to dielectric film A with high transmission to the wavelength band of 900 nm-1100 nm and high reflection to 1100 nm-1500 nm;

folding a mirror plating to dielectric film B with high transmission to the wavelength band of 900 nm-1100 nm and total reflection to 1100 nm-1500 nm;

outputting a mirror or a plating to dielectric film C with high transmission to the wavelength band of 900 nm-1100 nm and partial reflection to 1100-1200 nm; or a plating to dielectric film C with high transmission to the wavelength band of 900 nm-1200 nm and partial reflection to 1200 nm-1300 nm, or a plating to dielectric film C with high transmission to the wavelength band of 900 nm-1400 nm and partial reflection to 1400 nm-1500 nm.

suppressing an oscillation of radiation light by laser cavity coating, at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, further including:

when the pump light wavelength is 532 nm, the laser gain medium includes a Ti:sapphire crystal having a doping concentration of 0.1 at %-5 at %, the crystal surface of the laser gain medium is polished and incident light is incident on the crystal surface of the laser gain medium at a Brewster angle;

inputting a mirror plating to dielectric film A with high transmission to the wavelength band of 500-1100 nm and high reflection to 1100-1500 nm;

folding a mirror plating to dielectric film B with high transmission to the wavelength band of 500-1100 nm and full reflection to 1100-1500 nm;

outputting a mirror or a plating to dielectric film C with high transmission to the wavelength band of 500-1100 nm and partial reflection to 1100-1200 nm; or a plating to dielectric film C with high transmission to the wavelength band of 500-1200 nm and partial reflection to 1200-1300 nm, or a plating to dielectric film C with high transmission to the wavelength band of 500-1400 nm and partial reflection to 1400-1500 nm.

wherein, suppressing an oscillation of radiation light by laser cavity coating, at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, further including:

when the wavelength of the pump light is 795 nm, the laser gain medium includes yttrium aluminum garnet crystal with thulium doping concentration of 0.1 at %-20 at %, and the crystal surface of the laser gain medium is polished and plated with a dielectric film with high transmission to 795 nm and 1800-2100 nm bands;

inputting a mirror plating to dielectric film A with high transmission to the wavelength band of 795 nm and 1800-2100 nm high reflection to 2100-2500 nm;

folding a mirror plating to dielectric film B with high transmission to the wavelength band of 795 nm and 1800-2100 nm full reflection to 2100-2500 nm;

outputting a mirror or a plating to dielectric film C with high transmission to the wavelength band of 1800-2100 nm and partial reflection to 2100-2500 nm.

In the other aspect, a laser for breaking the limitation of fluorescence spectrum on laser wavelength is disclosed, wherein the laser includes a pumping source, an incident mirror, a laser gain medium, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the pump source is used for emitting pump light, and the incident mirror, the folding mirror and the exit mirror form a laser resonant cavity, the laser resonant cavity is used for regulating and controlling the oscillation of radiated light when electrons transition from high energy level to low energy level, at the same time, laser resonance is used to enhance the transition probability of electron-phonon coupling from high energy level to multi-phonon coupling; the tuning element is arranged in the laser resonant cavity at Brewster angle.

Preferably, the focusing system is further arranged between the pump source and the incident mirror.

Preferably, the tuning element includes a birefringence filter or prism.

Preferably, the surface of the laser gain medium is plated with a dielectric film with high transmission to a specific wavelength band.

Explanation of Terms of the Disclosure:

high reflectivity means that the reflectivity of incident light with a specific wavelength or band is greater than 99%;

high transmittance means that the transmittance of light with a specific wavelength or band is greater than 99%;

Partial reflection means that the reflectivity of light with a specific wavelength or band is between 80% and 99.9%.

According to the above technical scheme, the disclosure discloses a method and a laser for breaking through the limitation of fluorescence spectrum on laser wavelength, which have the following beneficial effects compared with the prior art:

according to the disclosure, the oscillation of radiated light when electrons transition from high energy level to low energy level is inhibited by using the coating regulation of the laser resonant cavity, and the transition probability of electron-phonon coupling energy level is enhanced when electrons transition from high energy level to multi-phonon coupling, that is, by coating the surfaces of the entrance mirror, folding mirror and exit mirror of the laser resonant cavity with dielectric films with high transmission or high reflection or partial transmission in a specific wavelength band, and matching with laser gain media and tuning elements, the limitation of fluorescence spectrum can be broken through, and laser with new wavelength can be obtained.

BRIEF DESCRIPTION OF THE DRAWINGS

In order to more clearly explain the embodiments of the present disclosure or the technical solutions in the prior art, the following will briefly introduce the drawings that need to be used in the description of the embodiments or the prior art. Obviously, the drawings in the following description are only the embodiments of the present disclosure. For those of ordinary skill in the art, other drawings can be obtained according to the provided drawings without any creative effort.

FIG. 1 is a schematic diagram of a laser structure provided by the present disclosure;

In the FIGURES: 1. pump source; 2. focusing system; 3. laser gain medium; 4. inputting mirror plated with dielectric film A; 5. folding mirror plated with dielectric film B; 6. output mirror plated with dielectric film C; 7. tuning element.

DETAILED DESCRIPTION OF THE EMBODIMENTS

In the following, technical solutions in the embodiment of the present disclosure will be clearly and completely described with reference to the accompanying drawings in the embodiment of the present disclosure, and it is obvious that the described embodiments are only a part of the embodiments of the present disclosure, but not all of the embodiments. Based on the embodiments of the present disclosure, all other embodiments obtained by those skilled in the art without making creative labor belong to the protection scope of the present disclosure.

On the one hand, the embodiment of the disclosure discloses a method for breaking through the limitation of fluorescence spectrum on laser wavelength. The method includes: in a laser gain medium, exciting electrons to a high energy level by pump light, and suppressing an oscillation of radiation light by laser cavity coating; at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, wherein the laser cavity includes an incident mirror, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the laser gain medium is located between an incident mirror and a folding mirror in the laser resonator.

The pump light can be provided by a pump source, and the pump light emitted by the pump source is focused by a focusing system and injected into a laser gain medium to excite the electron transition to a high energy level.

In that disclosure, through the physical effect of electron-phonon couple, a mode selection process of lase is utilized to realize excited radiation of electrons under the participation of multiple phonons, Therefore, it breaks through the traditional thinking and design thinking that the laser wavelength is limited by the fluorescent radiation envelope of the gain medium, and can be controlled by coating the laser cavity.

The method and process of the present disclosure will be described in detail through the following different embodiments:

Embodiment 1

The wavelength of the pump light emitted by the pump source is 976 nm, the pump source can be a semiconductor laser, the focusing system is composed of a pair of convex lenses with a focal length ratio of 1:1, the laser gain medium is a rare earth calcium borate crystal with a ytterbium ion doping concentration of 15 at %, and the surface of the crystal is polished and coated with a dielectric film with a high transmittance of 1000 nm to 1500 nm;

the laser resonator consists of an input mirror plated with a dielectric film A, a folding mirror plated with a dielectric film B, an output mirror plated with a dielectric film C, and the input mirror plated with a dielectric film A highly transmissive to 900-1100 nm and highly reflective to 1100-1500 nm;

fold-plated dielectric film B with high transmission to 900-1100 nm and total reflection to 1100-1500 nm;

the output mirror is coated with a dielectric film C that is highly transmissive to 900-1100 nm and partially reflective to 1100-1200 nm, the tuning element is a birefringent filter placed at Brewster's angle, and the tuned laser with wavelength from 1100-1200 nm can be output by rotating the tuning element;

if the output mirror is replaced by a dielectric film C coated with high transmission of 900-1200 nm and partial reflection of 1200-1300 nm, the tuned laser with wavelength of 1200-1300 nm can be output by rotating the tuning element;

if the output mirror is replaced by a dielectric film C coated with a high transmission of 900-1300 nm and a partial reflection of 1300-1400 nm, the tuned laser with a wavelength of 1300-1400 nm can be output by rotating the tuning element;

if a high transmission of 900-1400 nm and a partial reflection of 1400-1500 nm, the tuned laser with a wavelength of 1400-1500 nm can be output by rotating the tuning element.

Embodiment 2

The wavelength of the pump light emitted by the pump source is 532 nm, the pump source can be an all-solid-state laser, the focusing system is composed of a convex lens with a focal length of 50 mm, the laser gain medium is a Ti:sapphire crystal with a doping concentration of 0.5 at %, and the surface of the crystal is polished and Brewster's angle is placed in the resonant cavity.

The laser cavity consists of an input mirror coated with dielectric film A, a folded mirror coated with dielectric film B, an output mirror coated with dielectric film C, and the input mirror coated with dielectric film A highly transmitting to 500-1100 nm and highly reflecting to 1100-1500 nm;

fold-plated dielectric film B with high transmission to 500-1100 nm and total reflection to 1100-1500 nm;

The output mirror is coated with a dielectric film C that is highly transmissive to 500-1100 nm and partially reflective to 1100-1200 nm, and the tuning element is a birefringent filter placed at Brewster's angle; the rotating element can realize the output of tuned laser with wavelength of 1100-1200 nm;

If the output mirror is replaced by a dielectric film C coated with a high transmission of 500-1200 nm and a partial reflection of 1200-1300 nm, the tuned laser with a wavelength of 1200-1300 nm can be output by rotating the tuning element; the output mirror is replaced by a dielectric film C coated with a high transmission of 500-1300 nm and a partial reflection of 1300-1400 nm, and the tuned laser with a wavelength of 1300-1400 nm can be output by rotating the tuning element;

If the output mirror is replaced by a dielectric film C coated with a high transmission of 500-1400 nm and a partial reflection of 1400-1500 nm, the tuned laser with a wavelength of 1400-1500 nm can be output by rotating the tuning element.

Embodiment 3

The pump light emitted by the pump source is 795 nm, the pump source is a semiconductor laser, the focusing system is composed of a pair of convex lenses with a focal length ratio of 1:1, the laser gain medium is an yttrium aluminum garnet crystal with a thulium doping concentration of 10 at %, The crystal surface is polished and plated with high permeability dielectric films at 795 nm and 1800-2100 nm;

the laser resonator consists of an input mirror plated with a dielectric film A, a folding mirror plated with a dielectric film B, an output mirror plated with a dielectric film C, and the input mirror is plated with a dielectric film A having high transmission to 795 nm and 1800-2100 nm and high reflection to 2100-2500 nm;

the output mirror is coated with a dielectric film C which is highly transmissive to 795 nm and 1800-2100 nm and partially reflective to 2100-2500 nm, the tuning element is a prism placed at Brewster's angle, and the rotating tuning element can realize tuning laser output from 2100-2500 nm.

Embodiment 4

The pump light emitted by the pump source has a wavelength of 1.6 μm, the pump source is a fiber laser, and the fiber diameter is 200 μm. The focusing system is composed of a pair of convex lenses with a focal length ratio of 1:1. The laser gain medium is a Cr:ZnS crystal with a doping concentration of 10¹⁸/cm³, and the surface of the crystal is polished and plated with dielectric films with high transmission to 1600 nm and 2400-2800 nm;

The laser resonator consists of an input mirror coated with dielectric film A, a folding mirror coated with dielectric film B and an output mirror coated with dielectric film C;

an input mirror-plated dielectric film A with high transmission to 1600 nm and 2400-2800 nm and high reflection to 2800-3000 nm;

Fold-plated dielectric film B with high transmission at 1600 nm and 2400-2800 nm and high reflection and total reflection at 2800-3000 nm;

The output mirror is coated with a dielectric film C that is highly transmissive to 1600 nm and 2400-2800 nm and partially reflective to 2800-3000 nm. The tuning element is a prism placed at Brewster's angle, and the tuned laser with wavelength from 2800-3000 nm can be output by rotating the tuning element.

Embodiment 5

The wavelength of pump light emitted by the pump source is 1.0795 μm, and the pump source is Nd:YAP laser. The focusing system is composed of a convex lens with a focal length of 50 mm. The laser gain medium is NaCl(OH—):F²⁺ color center laser crystal. The crystal is placed in a clear crystal chamber cooled by liquid nitrogen at Brewster angle. The crystal chamber is kept in vacuum, and the crystal surface is polished and plated with 1080 and 1400-1800 nm pairs;

The laser resonant cavity consists of an input mirror coated with dielectric film A, a folding mirror coated with dielectric film B and an output mirror coated with dielectric film C. The input mirror is plated with a dielectric film A having high transmission to 1080 nm and 1400-1800 nm and high reflection to 1800-2000 nm.

The folded mirror is coated with a dielectric film B which is highly transmissive to 1080 nm and 1400-1800 nm and highly reflective and total-reflective to 1800-2000 nm;

The output mirror is coated with a dielectric film C with high transmission to 1080 nm and 1400-1800 nm and partial reflection to 1800-2000 nm. the tuning element is a prism placed at Brewster angle, and the rotating tuning element can realize the tunable laser output from 1800-2000 mm.

In the embodiment of the disclosure, the Brewster's angle placement of an element means that light rays are incident on the incident interface of the element at the Brewster's angle;

in the embodiment of the disclosure, dielectric film, dielectric film A, dielectric film B and dielectric film C are only used to distinguish dielectric films plated on different optical components.

As shown in FIG. 1 , another aspect of the present disclosure discloses a laser for breaking through the limitation of fluorescence spectrum on laser wavelength,

the laser includes a pump source 1, a focusing system 2, an entrance mirror 4 coated with dielectric film A, a laser gain medium 3, a folding mirror 5 coated with dielectric film B, a tuning element 7 and an output mirror 6 coated with dielectric film C, which are arranged in sequence along the optical path. the pump source 1 is used for emitting pump light of different wavelength bands, and the entrance mirror 4 coated with dielectric film A, the folding mirror 5 coated with dielectric film B and the output mirror 6 coated with dielectric film C film a laser resonant cavity; the laser resonant cavity is used to regulate and control the oscillation of radiated light when electrons transition from high energy level to low energy level, and at the same time, the transition probability of electron-phonon coupling energy level when electrons transition from high energy level to multi-phonon coupling is enhanced by laser resonance. The laser light reflected by the folding mirror 5 coated with dielectric film B enters the incident interface of the tuning element 7 at Brewster angle.

The tuning element 7 includes a birefringent filter or a prism.

In another embodiment, the surface of the laser gain medium 3 is plated with a dielectric film having high transmission to a specific wavelength band, so as to improve the passing efficiency of laser light.

In an embodiment, the gain medium is a laser gain medium having an electron-phonon coupling effect, It may be, but is not limited to, a single crystal or polycrystalline material that can provide lattice oscillation such as a laser crystal or laser ceramic doped with transition metals, rare earth luminescent ions, color centers, and the like.

In this specification, each embodiment is described in a progressive manner, and each embodiment focuses on the differences from other embodiments, and the same similar parts among the embodiments may be referred to each other. For the device disclosed in the embodiment, since it corresponds to the method disclosed in the embodiment, the description is relatively simple, and for the relevant points, refer to the description of the method part.

The foregoing description of the disclosed embodiments enables those skilled in the art to make or use the present disclosure. Various modifications to these embodiments will be apparent to those skilled in the art, and the general principles defined herein may be used without departing from the spirit or scope of the disclosure, In other embodiment implementing that. Accordingly, the present disclosure will not be limited to the embodiments shown herein, but will conform to the widest scope consistent with the principles and novel features disclosed herein. 

What is claimed is: 1-9. (canceled)
 10. A method for breaking a limitation of fluorescence spectrum on a laser wavelength, comprising: in a laser gain medium, exciting electrons to a high energy level by pump light, and suppressing an oscillation of radiation light by laser cavity coating, at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, wherein the laser cavity comprises an incident mirror, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the laser gain medium is located between an incident mirror and a folding mirror in the laser resonator, and the tuning element is arranged in the laser cavity at a Brewster angle.
 11. The method of claim 10, wherein the laser gain medium transits electrons to high energy level under the excitation of pump light, specifically comprising: focusing the pump light provided by the pump source by a focusing system and then injecting into the laser gain medium to excite the electron transition to the high energy level.
 12. The method of claim 10, wherein the laser resonance is used to enhance a transition probability of an electron-phonon coupling from high-energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of penetrating fluorescence spectrum and realize the oscillation of radiation light, specifically comprising: when the pump light wavelength is 976 nm, the laser gain medium comprises a crystal of calcium rare earth borate doped with ytterbium ions with a concentration of 1 at %-30 at %, and the crystal surface of the laser gain medium is polished and plated with a dielectric film with a high transmittance in the wavelength range of 1000 nm-1500 nm; the inputting mirror is plated with a dielectric film A with high transmission to the wavelength band of 900 nm-1100 nm and high reflection to 1100 nm-1500 nm; the folding mirror is plated with a dielectric film B with high transmission to the wavelength band of 900 nm-1100 nm and total reflection to 1100 nm-1500 nm; the exit mirror is plated with a dielectric film C with high transmission to the wavelength band of 900 nm-1100 nm and partial reflection to 1100-1200 nm; or plated with a dielectric film C with high transmission to the wavelength band of 900 nm-1200 nm and partial reflection to 1200 nm-1300 nm, or plated with a dielectric film C with high transmission to the wavelength band of 900 nm-1400 nm and partial reflection to 1400 nm-1500 nm.
 13. The method of claim 10, wherein suppressing an oscillation of radiation light by laser cavity coating, at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, further comprising: when the pump light wavelength is 532 nm, the laser gain medium comprises a Ti sapphire crystal having a doping concentration of 0.1 at %-5 at %, the crystal surface of the laser gain medium is polished and incident light is incident on the crystal surface of the laser gain medium at a Brewster angle; the incident mirror is plated with a dielectric film A with high transmission to the wavelength band of 500-1100 nm and high reflection to 1100-1500 nm; the folding mirror is plated with a dielectric film B with high transmission to the wavelength band of 500-1100 nm and total reflection to 1100-1500 nm; the exit mirror is plated with a dielectric film C with high transmission to the wavelength band of 500-1100 nm and partial reflection to 1100-1200 nm; or plated with a dielectric film C with high transmission to the wavelength band of 500-1200 nm and partial reflection to 1200-1300 nm, or plated with a dielectric film C with high transmission to the wavelength band of 500-1400 nm and partial reflection to 1400-1500 nm.
 14. The method of claim 10, wherein suppressing an oscillation of radiation light by laser cavity coating, at the same time, using a laser resonance to enhance a transition probability of an electron-phonon coupling from the high energy level to a multi-phonon coupling level, so as to realize the emission and enhancement of breakthrough fluorescence spectrum and realize the radiation light oscillation, further comprising: when the wavelength of the pump light is 795 nm, the laser gain medium comprises yttrium aluminum garnet crystal with thulium doping concentration of 0.1 at %-20 at %, and the crystal surface of the laser gain medium is polished and plated with a dielectric film with high transmission to wavelength band of 795 nm and 1800-2100 nm; the incident mirror is plated with a dielectric film A with high transmission to the wavelength band of 795 nm and 1800-2100 nm and high reflection to 2100-2500 nm; the folding mirror is plated with a dielectric film B with high transmission to the wavelength band of 795 nm and 1800-2100 nm and a total reflection to 2100-2500 nm; the exit mirror is plated with a dielectric film C with high transmission to the wavelength band of 1800-2100 nm and a partial reflection to 2100-2500 nm.
 15. A laser for breaking the limitation of fluorescence spectrum on laser wavelength of claim 10, wherein the laser comprises a pumping source, an incident mirror, a laser gain medium, a folding mirror, a tuning element and an exit mirror arranged in sequence along an optical path direction, the pump source is used for emitting pump light, and the incident mirror, the folding mirror and the exit mirror form a laser resonator; the laser resonator is used for regulating and controlling the oscillation of radiated light when electrons transition from high energy level to low energy level, at the same time, laser resonance is used to enhance the transition probability of electron-phonon coupling from high energy level to multi-phonon coupling; the tuning element is arranged in the laser resonator at Brewster angle.
 16. The laser of claim 15, wherein the focusing system is further arranged between the pump source and the incident mirror.
 17. The laser of claim 15, wherein the tuning element comprises a birefringence filter or prism.
 18. The laser of claim 15, wherein the surface of the laser gain medium is plated with a dielectric film with high transmission to a specific wavelength band. 